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Ordering of Elliptic Flow at High Pt. Zi-wei Lin The Ohio State University. Quark coalescence model v2 at high Pt: dominance of leading quark from phase space v2 from quarks to hadrons flavour ordering special cases, and the quark counting rule
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Ordering of Elliptic Flow at High Pt Zi-wei Lin The Ohio State University • Quark coalescence model • v2 at high Pt: • dominance of leading quark from phase space • v2 from quarks to hadrons • flavour ordering • special cases, and the quark counting rule • What have been neglected in the analysis? • Summary Z.W.L.&Ko,PRL89 Transverse Dynamics at RHIC BNL, March 2003
v2 data at low Pt v2 at a fixed pt follow mass scaling: v2(M) < v2(m) for M > m Huovinen et al, PLB503 STAR, PRL87
v2 data at high Pt (@130GeV) for identified hadrons: STAR, PRL89
v2 (@200GeV) for identified hadrons: Filimonov, QM02 see H. Huang, R. Snellings’s talks
Framework: the Quark Coalescence Model Near hadronization, gluon may decouple (decayed or absorbed), thus we may consider only constituent quarks just before the phase transition • for Multipliticy: coalescence factor (wavefunction) quark distributions (phase space) • Momentum distributions:
Dominance of the leading parton at high Ptfrom phase space Consider a formation of high Pt meson from a) a leading q and a soft qbar (~Pt+soft) b) q and qbar with equal momentum (Pt/2+Pt/2) If Pt/2 is still high, and only consider phase space: due to power-law enhancement of high Pt partons scenario a) dominates -aPt e n 1/Pt parton spectra just before phase transition
Parton v2 => hadron v2 if hadronic effects on v2 are neglected, then for mesons: leading q or qbar azimuthal angle w.r.t. reaction plane Ci: coalescence probability, for a high Pt parton to capture a soft parton i and form a hadron
for SU(3) hadrons at a fixed high Pt: same for all SU(3) hadrons at a given high Pt
Impose isospin symmetry & s-sbar symmetry: assume, for variables : At RHIC, pi+/pi-, K+/K-~1 depends on 2 ratios:
At RHIC, pbar/p~0.7 Further impose q-qbar symmetry: depends on 1 ratio: Flavour ordering at a fixed high Pt: gives • 2 independent relations (out of 3), can be checked using v2 of 4 particle species:
Several limits: Some limits: 1) leading light quark 2) leading s quark 3) Quark-counting rule
mass vs flavour ordering at low Ptat high Pt K curve will cross N & Lambda curves A schematic plot At high Pt:
Neglected in this analysis: • Independent fragmentation of parton jets -> may start to dominate at very high Pt • wavefunction overlap of coalescencing partons: (only phase space distributions are considered here) Ci: only depends on flavour i of the soft parton, not on flavour of the high pt parton or relative momenta Discussed recently by: Fries et al, nucl-th/0301087 Greco,Ko&Levai, nucl-th/0301093 Molnar&Voloshin, nucl-th/0302014 see D. Molnar, R. Fries’s talks
wavefunction overlap of coalescencing partons: 1) The limit of wide overlap (in relative momentum): -> phase space dominates -> flavour ordering 2) Wavefunction with exponential tail in radius: -> dipole-form power-law suppression -> qualitatively the same • 3) Gaussian wavefunction: -> exponential suppression of large relative momenta between coalescing quarks ->qualitatively different • 4) The limit of narrow overlap: baryon from 3 quarks of Pt/3, meson from 2 quarks of Pt/2 Molnar&Voloshin, nucl-th/0302014
Summary • Phase space consideration from the quark coalescence model: v2(high Pt) may follow flavour ordering instead of mass ordering for v2(low Pt) • If , all SU(3) hadrons have same v2 at a given high Pt • If , flavour ordering follows in isospin & quark-antiquark symmetric matter • The special case of corresponds to quark counting rule • Effects of wavefunctions (for the coalescence probability) and independent fragmentation can change the picture, recently discussed by several groups
v2 data at high Pt STAR, PRL90
Elliptic flow (v2): azimuthal asymmetry in transverse momentum Y X: impact parameter Z: beam axis
Elliptic Flow at Really High Momentum • STAR charged hadron elliptic flow out to pT = 12 GeV/c ! • finite v2 beyond pT = 6 GeV/c for semi-central • decrease of v2 in central? Peitzmann, QM02
Coalescence inALCOR Biro et al, PLB347; Biro, hep-ph/0005067; Zimanyi et al, Heavy Ion Phys4,15; PLB472, hep-ph/0103156 ALgebraic COalescence Rehadronization model Near hadronization, gluon may decouple (decayed or absorbed), thus consider only constituent q+qbar: coalescence factor 2Nf normalization factors, determined from 2Nf equations for quark # conservation: